Resumen Diseño de Maquinas de Shigley cap 2

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  • 8/5/2015

    1

    Chapter 2

    Materials

    Lecture Slides

    The McGraw-Hill Companies 2012

    Chapter Outline

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    Example 1-2

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    Solution

    Answer

    Answer

    Standard Tensile Test

    Used to obtain material characteristics and strengths Loaded in tension with slowly increasing P Load and deflection are recorded

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    Fig. 21

    Stress and Strain

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    The stress is calculated from

    where is the original cross-sectional area.

    The normal strain is calculated from

    where l0 is the original gauge length and l is the current length corresponding to the current P.

    Stress-Strain Diagram

    Plot stress vs. normal strain Typically linear relation until

    the proportional limit, pl No permanent deformation

    until the elastic limit, el Yield strength, Sy , defined at

    point where significant plastic deformation begins, or where permanent set reaches a fixed amount, usually 0.2% of the original gauge length

    Ultimate strength, Su , defined as the maximum stress on the diagram

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    Ductile material

    Brittle material

    Fig. 22

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    Elastic Relationship of Stress and Strain

    Slope of linear section is Youngs Modulus, or modulus of elasticity, E

    Hookes law

    E is relatively constant for a given type of material (e.g. steel, copper, aluminum)

    See Table A-5 for typical values

    Usually independent of heat treatment, carbon content, or alloying

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    Fig. 22 (a)

    True Stress-Strain Diagram Engineering stress-strain diagrams

    (commonly used) are based on original area.

    Area typically reduces under load, particularly during necking after point u.

    True stress is based on actual area corresponding to current P.

    True strain is the sum of the incremental elongations divided by the current gauge length at load P.

    Note that true stress continually increases all the way to fracture.

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    True Stress-strain

    Engineeringstress-strain

    (2-4)

    Compression Strength

    Compression tests are used to obtain compressive strengths. Buckling and bulging can be problematic. For ductile materials, compressive strengths are usually about

    the same as tensile strengths, Suc = Sut . For brittle materials, compressive strengths, Suc , are often

    greater than tensile strengths, Sut .

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    Torsional Strengths

    Torsional strengths are found by twisting solid circular bars. Results are plotted as a torque-twist diagram. Shear stresses in the specimen are linear with respect to the radial

    location zero at the center and maximum at the outer radius. Maximum shear stress is related to the angle of twist by

    q is the angle of twist (in radians) r is the radius of the bar l0 is the gauge length G is the material stiffness property called the shear modulus or

    modulus of rigidity.

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    Torsional Strengths

    Maximum shear stress is related to the applied torque by

    J is the polar second moment of area of the cross section For round cross section,

    Torsional yield strength, Ssy corresponds to the maximum shear stress at the point where the torque-twist diagram becomes significantly non-linear

    Modulus of rupture, Ssu corresponds to the torque Tu at the maximum point on the torque-twist diagram

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    Resilience

    Resilience Capacity of a material to absorb energy within its elastic range

    Modulus of resilience, uR Energy absorbed per unit

    volume without permanent deformation

    Equals the area under the stress-strain curve up to the elastic limit

    Elastic limit often approximated by yield point

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    Resilience Area under curve to yield point gives approximation

    If elastic region is linear,

    For two materials with the same yield strength, the less stiff material (lower E) has greater resilience

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    Toughness

    Toughness capacity of a material to absorb energy without fracture

    Modulus of toughness, uT Energy absorbed per unit volume

    without fracture Equals area under the stress-strain

    curve up to the fracture point

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    Toughness

    Area under curve up to fracture point

    Often estimated graphically from stress-strain data Approximated by using the average of yield and ultimate

    strengths and the strain at fracture

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    Resilience and Toughness

    Measures of energy absorbing characteristics of a material Units are energy per unit volume

    lbfin/in3 or J/m3 Assumes low strain rates For higher strain rates, use impact methods (See Sec. 2-5)

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    Statistical Significance of Material Properties

    Strength values are obtained from testing many nominally identical specimens

    Strength, a material property, is distributional and thus statistical in nature

    Example Histographic report for maximum stress of 1000 tensile tests on 1020 steel

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    Example for Statistical Material Property Histographic report for maximum stress of 1000 tensile tests on

    1020 steel

    Probability density number of occurrences divided by the total sample number

    Histogram of probability density for 1020 steel

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    Fig. 25

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    Example for Statistical Material Property Probability density function (See Ex. 20-4)

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    Fig. 25

    Statistical Quantity

    Statistical quantity described by mean, standard deviation, and distribution type

    From 1020 steel example: Mean stress = 63.62 kpsi Standard deviation = 2.594 kpsi Distribution is normal Notated as

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    Strengths from Tables

    Property tables often only report a single value for a strength term

    Important to check if it is mean, minimum, or some percentile Common to use 99% minimum strength, indicating 99% of the

    samples exceed the reported value

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    Cold Work Cold work Process of plastic

    straining below recrystallization temperature in the plastic region of the stress-strain diagram

    Loading to point i beyond the yield point, then unloading, causes permanent plastic deformation, p

    Reloading to point i behaves elastically all the way to i, with additional elastic strain e

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    Fig. 26 (a)

    Cold Work The yield point is effectively

    increased to point i Material is said to have been cold

    worked, or strain hardened Material is less ductile (more brittle)

    since the plastic zone between yield strength and ultimate strength is reduced

    Repeated strain hardening can lead to brittle failure

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    Fig. 26 (a)

    Reduction in Area

    Plot load P vs. Area Reduction Reduction in area corresponding to

    load Pf at fracture is

    R is a measure of ductility Ductility represents the ability of a

    material to absorb overloads and to be cold-worked

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    (2-12)

    Fig. 26 (b)

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    Cold-work Factor

    Cold-work factor W A measure of the quantity of cold work

    Shigleys Mechanical Engineering DesignFig. 26 (b)

    Equations for Cold-worked Strengths

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    Example 2-1

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    Example 2-1 (Continued)

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    Hardness

    Hardness The resistance of a material to penetration by a pointed tool

    Two most common hardness-measuring systems Rockwell A, B, and C scales Specified indenters and loads for each scale Hardness numbers are relative

    Brinell Hardness number HB is the applied load divided by the

    spherical surface area of the indentation

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    Strength and Hardness

    For many materials, relationship between ultimate strength and Brinell hardness number is roughly linear

    For steels

    For cast iron

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    Example 2-2

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    Impact Properties

    Charpy notched-bar test used to determine brittleness and impact strength

    Specimen struck by pendulum Energy absorbed, called impact value, is computed from height

    of swing after fracture

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    Effect of Temperature on Impact

    Some materials experience a sharp transition from ductile to brittle at a certain temperature

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    Fig. 27

    Effect of Strain Rate on Impact

    Average strain rate for stress-strain diagram is 0.001 in/(ins)

    Increasing strain rate increases strengths

    Due to yield strength approaching ultimate strength, a mild steel could be expected to behave elastically through practically its entire strength range under impact conditions

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    Fig. 28

    Temperature Effects on Strengths

    Plot of strength vs. temperature for carbon and alloy steels

    As temperature increases above room temperature Sut increase slightly, then

    decreases significantly Sy decreases continuously Results in increased

    ductility

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    Fig. 29

    Creep

    Creep a continuous deformation under load for long periods of time at elevated temperatures

    Often exhibits three stages 1st stage: elastic and plastic

    deformation; decreasing creep rate due to strain hardening

    2nd stage: constant minimum creep rate caused by the annealing effect

    3rd stage: considerable reduction in area; increased true stress; higher creep rate leading to fracture

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    Fig. 210

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    Material Numbering Systems

    Common numbering systems Society of Automotive Engineers (SAE) American Iron and Steel Institute (AISI) Unified Numbering System (UNS) American Society for Testing and Materials (ASTM) for cast

    irons

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    UNS Numbering System

    UNS system established by SAE in 1975 Letter prefix followed by 5 digit number Letter prefix designates material class

    G carbon and alloy steel A Aluminum alloy C Copper-based alloy S Stainless or corrosion-resistant steel

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    UNS for Steels For steel, letter prefix is G First two numbers indicate composition, excluding carbon content

    Second pair of numbers indicates carbon content in hundredths of a percent by weight

    Fifth number is used for special situations Example: G52986 is chromium alloy with 0.98% carbon

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    Some Casting Processes

    Sand Casting Shell Molding Investment Casting Powder-Metallurgy Process

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    Hot-working Processes

    Process in which metal is formed while heated above recrystallization temperature

    Refined grain size Rough surface finish Rolling, forging, extrusion, pressing Common bar cross-sections from hot-rolling

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    Fig. 211

    Cold-working Processes

    Forming of metal without elevating temperature

    Strain hardens, resulting in increase in yield strength

    Increases hardness and ultimate strength, decreases ductility

    Produces bright, smooth, reasonably accurate finish

    Cold-rolling used to produce wide flats and sheets

    Cold-drawing draws a hot-rolled bar through a smaller die

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    Fig. 212

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    Heat Treatment of Steel

    Time and temperature controlled processes that modifies material properties

    Annealing Heated above critical temperature, held, then slowly cooled Refines grain structure, softens, increases ductility Erases memory of prior operations Normalizing provides partial annealing by adjusting time and

    temperature Quenching

    Controlled cooling rate prevents full annealing Less pearlite, more martensite and/or bainite Increased strength, hardness, brittleness

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    Heat Treatment of Steel

    Tempering Reheat after quenching to a temperature below the critical

    temperature Relieves internal stresses Increases ductility, slight reduction in strength and hardness

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    Effects of Heat Treating

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    Fig. 213

    Case Hardening

    Process to increase hardness on outer surface, while retaining ductility and toughness in the core

    Addition of carbon to outer surface by exposure to high carbon solid, liquid, or gas at elevated temperature

    Can also achieve case hardening by heat treating only the outer surface, e.g. induction hardening or flame hardening

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    Alloy Steels

    Chromium Nickel Manganese Silicon Molybdenum Vanadium Tungsten

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    Corrosion-Resistant Steels

    Stainless steels Iron-base alloys with at least 12 % chromium Resists many corrosive conditions

    Four types of stainless steels Ferritic chromium Austenitic chromium-nickel Martensitic Precipitation-hardenable

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    Casting Materials

    Gray Cast Iron Ductile and Nodular Cast Iron White Cast Iron Malleable Cast Iron Alloy Cast Iron Cast Steel

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    Nonferrous Metals

    Aluminum Magnesium Titanium Copper-based alloys

    Brass with 5 to 15 percent zinc Gilding brass, commercial bronze, red brass

    Brass with 20 to 36 percent zinc Low brass, cartridge brass, yellow brass Low-leaded brass, high-leaded brass (engravers brass), free-

    cutting brass Admiralty metal Aluminum brass

    Brass with 36 to 40 percent zinc Muntz metal, naval brass

    Bronze Silcon bronze, phosphor bronze, aluminum bronze, beryllium

    bronzeShigleys Mechanical Engineering Design

    Plastics

    Thermoplastic any plastic that flows or is moldable when heat is applied

    Thermoset a plastic for which the polymerization process is finished in a hot molding press where the plastic is liquefied under pressure

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    Thermoplastic Properties (Table 2-2)

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    Thermoset Properties (Table 2-3)

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    Composite Materials

    Formed from two or more dissimilar materials, each of which contributes to the final properties

    Materials remain distinct from each other at the macroscopic level

    Usually amorphous and non-isotropic Often consists of laminates of filler to provide stiffness and

    strength and a matrix to hold the material together Common filler types:

    Shigleys Mechanical Engineering DesignFig. 214

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    Material Families and Classes (Table 2-4)

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    Material Families and Classes (Table 2-4)

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    Material Families and Classes (Table 2-4)

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    Material Families and Classes (Table 2-4)

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    Youngs Modulus for Various Materials

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    Fig. 215

    Youngs Modulus vs. Density

    Shigleys Mechanical Engineering DesignFig. 216

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    Specific Modulus

    Specific Modulus ratio of Youngs modulus to density, E /

    Also called specific stiffness Useful to minimize weight

    with primary design limitation of deflection, stiffness, or natural frequency

    Parallel lines representing different values of E / allow comparison of specific modulus between materials

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    Fig. 216

    Minimum Mass Guidelines for Youngs Modulus-Density Plot

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    Guidelines plot constant values of E/

    depends on type of loading

    = 1 for axial = 1/2 for

    bending

    Example, for axial loading,k = AE/l A = kl/Em = Al = (kl/E) l =kl2 /EThus, to minimize mass, maximize E/ ( = 1)

    Fig. 216

    The Performance Metric

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    The performance metric depends on (1) the functional requirements, (2) the geometry, and (3) the material properties.

    The function is often separable,

    f3 (M) is called the material efficiency coefficient.

    Maximizing or minimizing f3 (M) allows the material choice to be used to optimize P.

    Performance Metric Example

    Requirements: light, stiff, end-loaded cantilever beam with circular cross section

    Mass m of the beam is chosen as the performance metric to minimize

    Stiffness is functional requirement Stiffness is related to material and geometry

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    Performance Metric Example

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    From beam deflection table, 3

    3FlEI

    Sub Eq. (2-26) into Eq. (2-25) and solve for A

    The performance metric is

    Sub Eq. (2-27) into Eq. (2-28),

    Performance Metric Example

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    Separating into the form of Eq. (2-24),

    To minimize m, need to minimize f3 (M), or maximize

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    Performance Metric Example

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    M is called material index

    For this example, = Use guidelines parallel

    to E1/2/ Increasing M, move up

    and to the left Good candidates for this

    example are certain woods, composites, and ceramics

    Fig. 217

    Performance Metric Example

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    Additional constraints can be added as needed

    For example, if it is desired that E > 50 GPa, add horizontal line to limit the solution space

    Wood is eliminated as a viable option

    Fig. 218

    Strength vs. Density

    Shigleys Mechanical Engineering DesignFig. 219

    Specific Modulus

    Specific Strength ratio of strength to density, S /

    Useful to minimize weight with primary design limitation of strength

    Parallel lines representing different values of S / allow comparison of specific strength between materials

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    Fig. 219

    Minimum Mass Guidelines for Strength-Density Plot

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    Guidelines plot constant values of S/

    depends on type of loading

    = 1 for axial = 2/3 for bending

    Example, for axial loading, = F/A = S A = F/Sm = Al = (F/S) lThus, to minimize m, maximize S/ ( = 1)

    Fig. 219